These results can be modified to derive a robust detector that
accommodates small signals. To make this detector insensitive to
deviations from the nominal noise probability density, the
density should be replaced by the worst-case density consistent
with the maximum allowed deviations. For unimodal, symmetric
densities, the worst-case density equals that of the nominal
within a region centered about the origin while being
proportional to an exponential for values outside that region.
p
ω
nn=1-ε
p
o
nnif|n|<
n
′
1-ε
p
o
n
n
′
ⅇ-a|n|-
n
′
if|n|>
n
′
p
ω
n
n
1
ε
p
o
n
n
n
n
′
1
ε
p
o
n
n
′
a
n
n
′
n
n
′
The parameter aa controls the rate
of decrease of the exponential tail; it is specifies by requiring
that the derivative of the density's logarithm be continuous at
n=
n
′
n
n
′
. Thus,
a=-ddnln
p
o
nn
a
n
p
o
n
n
for
n=
n
′
n
n
′
. For the worst-case density to be a probability
density, the boundary value
n
′
n
′
and the deviation parameter εε
must be such that its integral is unity. As
εε is fixed, this requirement
reduces to a specification of
n
′
n
′
.
∫-
n
′
n
′
p
o
nndn+2a
p
o
n
n
′
=11-ε
n
n
′
n
′
p
o
n
n
2
a
p
o
n
n
′
1
1
ε
For the case where the nominal density
a=
n
′
σ2
a
n
′
σ
2
and this equation becomes
1-2Q
n
′
σ+σ
n
′
2πⅇ-
n
′
22σ2+11-ε
1
2
Q
n
′
σ
σ
n
′
2
n
′
2
2
σ
2
1
1
ε
The non-linearity required by the small-signal detection
strategy thus equals the negative derivative of the logarithm of
the worst-case density within the boundaries while equaling a
constant outside that region.
frl=-ddnln
p
o
nn|n=rlif|rl|<
n
′
asignrlif|rl|>
n
′
f
r
l
n
r
l
n
p
o
n
n
r
l
n
′
a
sign
r
l
r
l
n
′
(1)
The robust detector for small signals thus consists of a clipper
followed by a matched filter for each signal, the results of
which are compared with a threshold.